{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":1,"startPagecode":1},"records":[{"abstractinfo":"选择<span style=\"color:red\">长岛</span>典型的两个旅游景点的岩石和岸滩附着的8个溢油样品，对样品中的饱和烷烃、萜烷、甾烷及多环芳烃化合物的分布特征及典型生物标志物诊断比值进行了比对分析。 t检验结果表明，置信度为95％时，8个油样的生物标志物诊断比值指标均不能够完全匹配，不可判定其来自同一油源。九丈崖溢油样品之间差异性高于月牙湾。可见，<span style=\"color:red\">长岛</span>九丈崖岩石和月牙湾岸滩附着溢油样品之间具有较大相似度，但指纹特征各不相同，部分样品差别较大，具有混合油的指纹特征，为多次溢油的混合油样。","authors":[{"authorName":"韩彬","id":"e046aeb9-3377-4cf0-8ecc-1eff0309eb0d","originalAuthorName":"韩彬"},{"authorName":"杨佩华","id":"8c0f762f-7070-4a35-81ce-5165bbc87502","originalAuthorName":"杨佩华"},{"authorName":"高伟","id":"df326e08-6fb0-44f5-8942-5ccc6a538426","originalAuthorName":"高伟"},{"authorName":"郑立","id":"8a771040-4cf0-4ab1-be1e-740d09ba760b","originalAuthorName":"郑立"},{"authorName":"王小如","id":"be690fdc-588d-46d4-8a98-ba365b57a725","originalAuthorName":"王小如"},{"authorName":"王江涛","id":"9ddeb55d-0960-42f6-a421-fffcdfb467e3","originalAuthorName":"王江涛"}],"doi":"10.7524/j.issn.0254-6108.2015.04.2014082801","fpage":"718","id":"d6ee39f7-e9aa-445c-95f3-6c52e0a07fef","issue":"4","journal":{"abbrevTitle":"HJHX","coverImgSrc":"journal/img/cover/HJHX.jpg","id":"43","issnPpub":"0254-6108","publisherId":"HJHX","title":"环境化学   "},"keywords":[{"id":"048d8fc9-440a-4daa-908b-46e7af5d592e","keyword":"<span style=\"color:red\">长岛</span>","originalKeyword":"长岛"},{"id":"104f408f-bb28-4bc9-ab1b-9cc8da53cac3","keyword":"岸滩","originalKeyword":"岸滩"},{"id":"8ee31625-978f-4aa3-ba02-06cdad141fc8","keyword":"溢油","originalKeyword":"溢油"},{"id":"1700641d-8bf0-40bf-842e-adbb63391f25","keyword":"混合油","originalKeyword":"混合油"},{"id":"e657b795-0ab3-43c5-a3e8-3127d679eade","keyword":"指纹","originalKeyword":"指纹"}],"language":"zh","publisherId":"hjhx201504015","title":"<span style=\"color:red\">长岛</span>岸滩及岩石附着油污指纹特征比对","volume":"","year":"2015"},{"abstractinfo":"采用反应射频磁控溅射技术, 在非晶石英衬底上不同温度下制备了纳米多晶Gd掺杂CeO<SUB>2</SUB>(简称GDC)氧离子导体电解质薄膜, 采用X射线衍射仪、原子力显微镜对薄膜物相、晶粒大小、生长形貌进行了表征, 利用交流阻抗谱仪测试了GDC薄膜的电学性能. 结果表明, GDC薄膜生长取向随沉积温度而变化: 300～400℃时为强(111)织构生长, 而500～600℃时薄膜趋于无规则生长; 随着沉积温度的升高, 薄膜的生长形貌由同一取向的大棱形生<span style=\"color:red\">长岛</span>转变为密集球形小生<span style=\"color:red\">长岛</span>; GDC多晶薄膜的电导活化能约为1.3eV, 接近于晶界电导活化能值, 说明GDC交流阻抗主要源于晶界的贡献; 晶界空间电荷效应导致GDC薄膜电导率随晶粒尺寸而变化, 晶粒尺寸越小, 电导率越大.","authors":[{"authorName":"马小叶","id":"81f2ba36-cfb3-49ca-b29d-134ba9ea9afb","originalAuthorName":"马小叶"},{"authorName":"姜雪宁","id":"20d925c9-6834-4132-af64-dc13b4bd905b","originalAuthorName":"姜雪宁"},{"authorName":"孟宪芹","id":"9619319c-9351-4dd1-921e-2b10b3753e52","originalAuthorName":"孟宪芹"},{"authorName":"庞胜利","id":"aaf867cf-8e6b-47ee-aabd-91572f311f75","originalAuthorName":"庞胜利"},{"authorName":"孟昕","id":"e6054049-b6fa-4302-87e1-679b7212de53","originalAuthorName":"孟昕"},{"authorName":"张庆瑜","id":"b7930fcc-c05d-4aa6-be34-5011d67ff633","originalAuthorName":"张庆瑜"}],"categoryName":"|","doi":"10.3724/SP.J.1077.2008.00912","fpage":"912","id":"673e5635-1950-48ae-83ec-655e23c16307","issue":"5","journal":{"abbrevTitle":"WJCLXB","coverImgSrc":"journal/img/cover/WJCLXB.jpg","id":"62","issnPpub":"1000-324X","publisherId":"WJCLXB","title":"无机材料学报"},"keywords":[{"id":"22fce051-a951-448e-aadd-947650c6286e","keyword":"Gd掺杂CeO<SUB>2</SUB>电解质薄膜","originalKeyword":"Gd掺杂CeO<SUB>2</SUB>电解质薄膜"},{"id":"1f90c04f-b162-42a6-a7a9-0ffa66ffdf14","keyword":" reactive magnetron sputtering","originalKeyword":" reactive magnetron sputtering"},{"id":"a3802cb4-1379-4e42-be01-c98a56a1e876","keyword":" film growth","originalKeyword":" film growth"},{"id":"5b2281ac-bd2b-460f-8de0-0da1a9610da2","keyword":" electrical properties","originalKeyword":" electrical properties"}],"language":"zh","publisherId":"1000-324X_2008_5_32","title":"沉积温度对Gd掺杂CeO<SUB>2</SUB>电解质薄膜生长及电学特性的影响","volume":"23","year":"2008"},{"abstractinfo":"采用反应射频磁控溅射技术,在非晶石英衬底上不同温度下制备了纳米多晶Gd掺杂CeO2(简称GDC)氧离子导体电解质薄膜,采用X射线衍射仪、原子力显微镜对薄膜物相、晶粒大小、生长形貌进行了表征,利用交流阻抗谱仪测试了GDC薄膜的电学性能.结果表明,GDC薄膜生长取向随沉积温度而变化:300-400℃时为强(111)织构生长,而500-600℃时薄膜趋于无规则生长;随着沉积温度的升高,薄膜的牛长形貌由同一取向的大棱形生<span style=\"color:red\">长岛</span>转变为密集球形小生<span style=\"color:red\">长岛</span>;GDC多晶薄膜的电导活化能约为1.3eV,接近于晶界电导活化能值,说明GDC交流阻抗主要源于晶界的贡献;晶界空间电荷效应导致GDC薄膜电导率随晶粒尺寸而变化,晶粒尺寸越小,电导率越大.","authors":[{"authorName":"马小叶","id":"ba7ca073-1d25-4a95-af6c-754b82eb07d4","originalAuthorName":"马小叶"},{"authorName":"姜雪宁","id":"320cd07d-7e4c-437f-beb1-cd250fdff3e8","originalAuthorName":"姜雪宁"},{"authorName":"孟宪芹","id":"db08a677-19e5-43e6-8a76-cd6651857f53","originalAuthorName":"孟宪芹"},{"authorName":"庞胜利","id":"d3b225bb-49a4-4336-a458-080e1fbfebea","originalAuthorName":"庞胜利"},{"authorName":"孟昕","id":"5f5239da-20e3-490b-9f20-758bd14980a0","originalAuthorName":"孟昕"},{"authorName":"张庆瑜","id":"9fa59607-fa46-43da-92f5-bdeada44a275","originalAuthorName":"张庆瑜"}],"doi":"10.3321/j.issn:1000-324X.2008.05.010","fpage":"912","id":"2ca82b1f-3edd-448a-8314-68dbf6e130b5","issue":"5","journal":{"abbrevTitle":"WJCLXB","coverImgSrc":"journal/img/cover/WJCLXB.jpg","id":"62","issnPpub":"1000-324X","publisherId":"WJCLXB","title":"无机材料学报"},"keywords":[{"id":"6205a824-a79d-408b-a322-ed6f42be56e9","keyword":"Gd掺杂CeO2电解质薄膜","originalKeyword":"Gd掺杂CeO2电解质薄膜"},{"id":"d794c3ee-f802-40f4-9952-ff9a400e6955","keyword":"反应磁控溅射","originalKeyword":"反应磁控溅射"},{"id":"c847dd25-f775-481d-9c44-6ee2e8f589cc","keyword":"薄膜生长","originalKeyword":"薄膜生长"},{"id":"8155f53c-3e68-48cc-aae2-3db508f3e527","keyword":"电学特性","originalKeyword":"电学特性"}],"language":"zh","publisherId":"wjclxb200805010","title":"沉积温度对Gd掺杂CeO2电解质薄膜生长及电学特性的影响","volume":"23","year":"2008"},{"abstractinfo":"采用反应射频磁控溅射技术在(0001)蓝宝石基片上制备了不同调制结构的(GDC/YSZ)12多层氧离子导体电解质薄膜.利用电子探针微区分析技术测得薄膜的摩尔质量比为m(Zr):m(Y)=5.73:1、m(Ce):m(Gd)=4.12:1;X射线衍射(XRD)与小角X射线反射(XRR)结果表明,GDC/YSZ调制比为5:1、2:1和1:2的样品(A1～A3)具有好的超晶格结构,而A4样品未形成超晶格结构;原子力显微镜形貌分析结果表明多层膜呈密集岛状生长形貌,与GDC、YSZ单层膜比较,多层膜生<span style=\"color:red\">长岛</span>尺寸减小,密度增大,表面粗糙度明显减小;电学性能测试与理论分析结果表明,界面缺陷使多层膜电导率提高,而GDC成分增多,则超晶格多层膜电导率增大.","authors":[{"authorName":"孟昕","id":"f769ed7c-aa3f-4b64-9f28-5bdcf5bb624d","originalAuthorName":"孟昕"},{"authorName":"孟宪芹","id":"26924275-56da-4c31-b768-f4319bf5f6bc","originalAuthorName":"孟宪芹"},{"authorName":"姜雪宁","id":"8e623d07-cff5-4e89-9122-f85536d73f77","originalAuthorName":"姜雪宁"},{"authorName":"庞胜利","id":"05820459-e8a2-4f33-9d7d-8038679ef178","originalAuthorName":"庞胜利"},{"authorName":"李向楠","id":"95c2b623-99b1-40ea-b519-2097717855a2","originalAuthorName":"李向楠"},{"authorName":"张庆瑜","id":"f3b8af31-f514-4056-b482-9c4d3d255e11","originalAuthorName":"张庆瑜"}],"doi":"","fpage":"1120","id":"8ac7d7b3-54c9-4a97-85b1-f52349941b59","issue":"7","journal":{"abbrevTitle":"GNCL","coverImgSrc":"journal/img/cover/GNCL.jpg","id":"33","issnPpub":"1001-9731","publisherId":"GNCL","title":"功能材料"},"keywords":[{"id":"94852711-65d8-4cf9-a8a3-b6cf4854b08f","keyword":"GDC/YSZ多层薄膜","originalKeyword":"GDC/YSZ多层薄膜"},{"id":"0acb9669-4a94-495c-a1ab-cbce62be2472","keyword":"结构","originalKeyword":"结构"},{"id":"89b9a761-4ec7-450a-889d-76c419b23b65","keyword":"表面形貌","originalKeyword":"表面形貌"},{"id":"b5f45e25-700a-4e30-a73a-321aee9d20ec","keyword":"电学性质","originalKeyword":"电学性质"}],"language":"zh","publisherId":"gncl201007003","title":"调制比对GDC/YSZ多层氧离子导体薄膜结构与电学性能的影响","volume":"41","year":"2010"},{"abstractinfo":"采用FactSage热力学软件和镁基数据库计算了Mg-6Zn-1Y合金的凝固路径.利用SEM并配合EDS,XRD,DSC研究了超高压下Mg-6Zn-1Y合金的凝固过程和准晶形成.结果表明:常压下该合金凝固组织主要由粗大a-Mg枝晶和分布在枝晶间含准晶I-Mg3YZn6相的层片状组织等组成,合金凝固过程的实验分析与热力学计算结果吻合较好.Mg-6Zn-1Y合金在GPa级超高压下凝固不但可以获得超细的枝晶组织,还可改善枝晶间层片状组织的形态.随着凝固压力的增加,由常压下的晶间网状或带状逐渐过渡到超高压下的“<span style=\"color:red\">长岛</span>状”以及“粒状”.特别是提高了单位面积上晶间相(含准晶I-Mg3YZn6相)的含量,其体积分数约占40％,同时还形成了纳米级的弥散分布在基体上高Y含量的Mg-Zn-Y三元新相.","authors":[{"authorName":"董允","id":"2c03e602-41eb-49b7-9057-7b89fe76f87c","originalAuthorName":"董允"},{"authorName":"林小娉","id":"1799fc55-41f7-4939-99d5-d9a4720f22a2","originalAuthorName":"林小娉"},{"authorName":"徐瑞","id":"6cd18039-2e5c-4013-b143-f2f8e15e2cc8","originalAuthorName":"徐瑞"},{"authorName":"刘士俊","id":"96350ae8-13cf-4ca6-8729-6dd4a2a77ed2","originalAuthorName":"刘士俊"},{"authorName":"田莎莎","id":"b90d2c67-47c2-4025-b2da-5b64bef032e0","originalAuthorName":"田莎莎"}],"doi":"","fpage":"1117","id":"b4da8b9a-db04-4a99-a4b8-b60ae3031b67","issue":"5","journal":{"abbrevTitle":"XYJSCLYGC","coverImgSrc":"journal/img/cover/XYJSCLYGC.jpg","id":"69","issnPpub":"1002-185X","publisherId":"XYJSCLYGC","title":"稀有金属材料与工程"},"keywords":[{"id":"7ccb62a7-6805-4699-8286-0fda0c1eb697","keyword":"GPa级超高压","originalKeyword":"GPa级超高压"},{"id":"431b0fd4-8360-4748-b840-480c2d517f66","keyword":"Mg-6Zn-1Y合金","originalKeyword":"Mg-6Zn-1Y合金"},{"id":"d6e3d00d-f4d4-4ec6-a260-95596bbdbf66","keyword":"准晶","originalKeyword":"准晶"},{"id":"62b7fdde-783f-4fe3-b705-00622ed392ca","keyword":"枝晶组织","originalKeyword":"枝晶组织"}],"language":"zh","publisherId":"xyjsclygc201405018","title":"GPa级超高压下Mg-6Zn-1Y合金凝固过程及准晶形成","volume":"43","year":"2014"}],"totalpage":1,"totalrecord":5}